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05/29/08 - USPTO Class 336 |  107 views | #20080122569 | Prev - Next | About this Page  336 rss/xml feed  monitor keywords

Coil structure for high frequency transformer

USPTO Application #: 20080122569
Title: Coil structure for high frequency transformer
Abstract: The present invention provides a continuous conductive planar coil structure. The continuous conductive planar coil structure includes a first output terminal, a second output terminal, a coil body and a projection plane parallel to the coil body, wherein a first projection on the projection plane is formed by the first output terminal, a second projection on the projection plane is formed by the second output terminal, and an overlapping portion is between the first projection and the second projection. (end of abstract)



Agent: Volpe And Koenig, P.C. - Philadelphia, PA, US
Inventors: Hao-Yi Ye, Jia-Ping Chen, Hong-Shan Tao, Jian-Ping Ying, Zhong Chen, Jing-Fei He, Feng Li, Hong-Jian Gan
USPTO Applicaton #: 20080122569 - Class: 336223 (USPTO)

Coil structure for high frequency transformer description/claims


The Patent Description & Claims data below is from USPTO Patent Application 20080122569, Coil structure for high frequency transformer.

Brief Patent Description - Full Patent Description - Patent Application Claims
  monitor keywords FIELD OF THE INVENTION

This invention relates to a continuous conductive planar coil structure, and more particularly to a coil structure for a high efficiency transformer.

BACKGROUND OF THE INVENTION

As most electrical power products, the development trend of a DC/DC converter is to form a converter with high efficiency, high power density, high reliability and low cost.

For a DC/DC converter outputting low voltage and high current, it is important to optimize the design of a transformer in order to meet the above-mentioned development trend. And due to the requirement of high efficiency at higher and higher output current, the secondary side coil of a transformer is changed from conventional winding type coil to a strip type continuous conductive planar type coil.

Please refer to FIG. 1, which is disclosed in U.S. Pat. No. 6,577,220 to show a perspective view of coil structure. As shown in FIG. 1, the coil structure 1 is made by folding a strip type continuous conductive structure. In comparison with the conventional winding type structure, the coil structure shown in FIG. 1 has a reduced DC resistance and an increased heat-dissipating area, so that the conduction loss of the transformer is significantly reduced.

For high power density, the switching frequency of a circuit is increased so as to reduce the volume of a magnetic component. However, there are some problems when the coil structure shown in FIG. 1 is used in a high frequency condition.

With the increasing frequency, the skin effect and the proximity effect of the AC current in a conductor are more severe, so that the AC loss is correspondingly increased. In addition, the electromagnetic radiation will generate from a circuit owing to the improper layout, so that the power density and the reliability are disadvantageously affected owing to the electromagnetic interferences.

When the coil structure shown in FIG. 1 is used in the high frequency condition, high frequency current with reverse directions flow through the output terminals (such as output terminals 11, 12) of the coil structure. When the output terminals are very close, current concentrates on the two sides proximate each other owing to the coupling of electromagnetic fields therebetween, which is the proximity effect, and therefore the current is distributed unevenly which increases the power loss. Furthermore, there is an interval 10 between the two output terminals 11 and 12, so that there is the electromagnetic interference produced from the interval 10 to surroundings, and the circuit is also interfered with the electromagnetic radiation in the surroundings.

Please refer to FIG. 2, which is a block diagram showing a DC/DC converter according to the prior art. In FIG. 2, the DC/DC converter includes an input circuit 21, a transformer 22 and an output circuit 23. In addition, there are two output terminals 24 and 25 on the secondary side of the transformer 22, and a loop 26 is formed by the output terminals 24, 25 and the output circuit 23. The current doubler rectifier circuit, the voltage doubler rectifier circuit, the full-bridge rectifier circuit and the half-wave rectifier circuit have the above-mentioned structures, and the characteristics thereof are those the current flowing into the output terminal 24 of the transformer 22 has the identical quantities and reverse directions with the current flowing out of the output 25 of the transformer 22, and the current in the loop 26 is high efficiency AC current. According to the electromagnetic field theory, the loop passing the high frequency AC current therethrough produces the high frequency magnetic field (magnetic field H in FIG. 2), which emits the electromagnetic wave to interfere surroundings. In addition, the electromagnetic radiation in the surroundings can also be received by the loop 26, so as to interfere the circuit itself. Therefore, in order to reduce the electromagnetic radiation in the surroundings and to reduce the interference in the circuit, the area of the loop 26 should be significantly reduced.

Please refer to FIG. 3, which is a block diagram showing another DC/DC converter according to the prior art. In FIG. 3, the DC/DC converter 3 includes an input circuit 31, a transformer 32 and an output circuit 33. In FIG. 3, the transformer 32 has a center-tapped structure, and there are three output terminals 34, 35 and 36 on the secondary side of the transformer 32. The first loop 37 is formed by the output terminals 35, 36 and the output circuit 33 on the secondary side of the transformer 32. The second loop 38 is formed by the output terminals 34, 36 and the output circuit 33 on the secondary side of the transformer 32. The third loop 39 is formed by the output terminals 34, 35 and the output circuit 33.

When the current is flowing in one (such as the loop 37) of the loops, the current flowing in the output terminal 35 and the current flowing out of the output terminal 36 have identical quantities and reverse directions. When the current flows in the loop 38, the current in the output terminal 34 and the current in the output terminal 36 have identical quantities and reverse directions. The current in the output terminal 34 and the current in the output terminal 35 have identical quantities and the phase difference of 180°. And the odd-order harmonics of the AC component of the current in the output terminal 34 and 35 have identical quantities and reverse directions. The center tapped full-wave rectifier circuit has the above-mentioned structure. Similarly, in order to reduce the electromagnetic radiation in the surroundings and to reduce the interference in the circuit, the areas of the loops 37, 38 and 39 should be significantly reduced, i.e. the outputs 34, 35 and 36 should be very close which can also alleviate the unevenly distribution of the current due to proximity effect.

Please refer to FIG. 4(a) showing a voltage type full-wave rectifier circuit according to the prior art. As shown in FIG. 4(a), the full-wave rectifier circuit 4 includes switches S1, S2 connected to the secondary side of the transformer T and connected to the output inductor L, wherein the output inductor L is connected to the positive terminal of the output capacitor Co, and the negative terminal of the output capacitor Co is connected to the center tap on the secondary side of the transformer T.

When the full-wave rectifier circuit shown in FIG. 4(a) is used in a pulse width modulation (PWM) circuit, the waveforms of the current passing through the switches and the center tap (i.e. the output inductor L) is shown in FIG. 4(b).

In FIG. 4(b), the current passing through the switch S1 is denoted as i1, the current passing through the switch S2 is denoted as i2, and the current passing the center tap is denoted as i3.

FIG. 4(c) is a diagram showing the harmonic spectra of the current i3. FIG. 4(d) is a diagram showing the harmonic spectra of the currents i1 and i2 passing through the switches S1 and S2. FIG. 4(c) and FIG. 4(d) show a ratio of the harmonic frequency to the switch frequency versus a ratio of the harmonic amplitude to the output current. As shown in FIGS. 4(c) and 4(d), the AC component of the current i3 is a very small part of the total current and has the even-order harmonics, and the odd-order harmonic of the current passing through the switches S1 and S2 is the major part of the total current.

Therefore, there is a need to provide different coil structures for secondary side rectification circuits of various transformers in order to overcome the aforesaid drawbacks of the transformer used in the high frequency condition.

Accordingly, in order to overcome the disadvantages of the prior art described above, the present invention provides a continuous conductive planar coil structure for a high frequency transformer.

SUMMARY OF THE INVENTION

It is an aspect of the present invention to provide a continuous conductive planar coil structure. The continuous conductive planar coil structure includes a first output terminal, a second output terminal, a coil body and a projection plane parallel to the coil body, wherein a first projection on the projection plane is formed by the first output terminal, a second projection on the projection plane is formed by the second output terminal, and an overlapping portion is formed by the first projection and the second projection.

Preferably, the first projection has a first area, the second projection has a second area, the overlapping portion has a third area, and one of a ratio of the third area to the first area and a ratio of the third area to the second area is more than 10%.

Preferably, a third projection on the projection plane is formed by the coil body, and a fourth projection is formed by the first projection and the second projection, wherein a first boundary is between the fourth projection and the third projection, the fourth projection has a second boundary, the first boundary and the second boundary intersect at a first point and a second point, the third projection is symmetric relatively to a first axis passing through the fourth projection, a second axis parallel to the first axis passes through the first point, and a third axis parallel to the first axis passes through the second point. The continuous conductive planar coil structure further includes a first switch having a first end connected to the first output terminal and having a projection with a third boundary on the projection plane, a second switch having a second end connected to the second output terminal and having a projection with a fourth boundary on the projection plane, wherein a horizontal line perpendicular to the first axis crosses one of the third boundary and the fourth boundary, and a distance between the first horizontal line and the first point is relatively minimal. The continuous conductive planar coil structure further includes a fifth projection demarcated by the first boundary, the second axis, the third axis and the first horizontal line, and a ratio of an area of the overlapping portion to an area of the fifth projection being more than 5%.

Preferably, the continuous conductive planar coil structure includes a sixth projection demarcated by the first boundary, the second boundary, the second axis, the third axis and the horizontal line, and a ratio of the area of the overlapping portion to an area of the sixth projection is more than 5%.



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